# 3.9: Lossless and Low-Loss Transmission Lines

- Page ID
- 24221

Quite often the loss in a transmission line is small enough that it may be neglected. In this case, several aspects of transmission line theory may be simplified. In this section, we present these simplifications.

First, recall that “loss” refers to the reduction of magnitude as a wave propagates through space. In the lumped-element equivalent circuit model (Section 3.4), the parameters \(R'\) and \(G'\) of the represent physical mechanisms associated with loss. Specifically, \(R'\) represents the resistance of conductors, whereas \(G'\) represents the undesirable current induced between conductors through the spacing material. Also recall that the propagation constant \(\gamma\) is, in general, given by \[\gamma \triangleq \sqrt{\left(R'+j\omega L'\right)\left(G'+j\omega C'\right)}\]

With this in mind, we now define “low loss” as meeting the conditions: \[R'\ll\omega L' \label{m0083_eLLR}\] \[G'\ll\omega C' \label{m0083_eLLG}\] When these conditions are met, the propagation constant simplifies as follows:

\begin{aligned}

\gamma & \approx \sqrt{\left(j \omega L^{\prime}\right)\left(j \omega C^{\prime}\right)} \\

&=\sqrt{-\omega^{2} L^{\prime} C^{\prime}} \\

&=j \omega \sqrt{L^{\prime} C^{\prime}}

\end{aligned}

and subsequently

\begin{align}

\alpha &\triangleq \operatorname{Re}\{\gamma\} \approx 0 && \text { (low-loss approx.) }\\

\beta &\triangleq \operatorname{Im}\{\gamma\} \approx \omega \sqrt{L^{\prime} C^{\prime}} &&\text { (low-loss approx.) } \\

v_{p} &=\omega / \beta \approx \frac{1}{\sqrt{L^{\prime} C^{\prime}}} &&\text { (low-loss approx.) }

\end{align}

Similarly: \[Z_0 = \sqrt{\frac{R' + j\omega L'}{G' + j\omega C'}} \approx \sqrt{\frac{L'}{C'}} ~~~ \mbox{(low-loss approx.)}\]

Of course if the line is strictly lossless (i.e., \(R'=G'=0\)) then these are not approximations, but rather the exact expressions.

In practice, these approximations are quite commonly used, since practical transmission lines typically meet the conditions expressed in Inequalities \ref{m0083_eLLR} and \ref{m0083_eLLG} and the resulting expressions are much simpler. We further observe that \(Z_0\) and \(v_p\) are approximately independent of frequency when these conditions hold.

However, also note that “low loss” does not mean “no loss,” and it is common to apply these expressions even when \(R'\) and/or \(G'\) is large enough to yield significant loss. For example, a coaxial cable used to connect an antenna on a tower to a radio near the ground typically has loss that is important to consider in the analysis and design process, but nevertheless satisfies Equations \ref{m0083_eLLR} and \ref{m0083_eLLG}. In this case, the low-loss expression for \(\beta\) is used, but \(\alpha\) might not be approximated as zero.

## Contributors and Attributions

Ellingson, Steven W. (2018) Electromagnetics, Vol. 1. Blacksburg, VA: VT Publishing. https://doi.org/10.21061/electromagnetics-vol-1 Licensed with CC BY-SA 4.0 https://creativecommons.org/licenses/by-sa/4.0. Report adoption of this book here. If you are a professor reviewing, adopting, or adapting this textbook please help us understand a little more about your use by filling out this form.